supplementary materials


Acta Cryst. (2007). E63, o3357    [ doi:10.1107/S1600536807030772 ]

(E)-N-(1,3-Oxazolidin-2-ylidene)benzamide

H.-G. An

Abstract top

The aryl and oxazolidine rings in the title compound, C10H10N2O2, are essentially coplanar [dihedral angle = 3.8 (6)°]. The crystal structure involves intra- and intermolecular N-H...O hydrogen bonds.

Comment top

The X-ray crystallographic structure of the title compound, (I) (Fig. 1), has not been published previously, although the deprotonated molecule has been reported in two metal complexes, namely, trans-bis(2-benzamido)oxazoline metal(II) where M = Ni (Jiang et al., 2006) and M = Cu (Zhang et al., 2004).

The bond lengths and angles have the usual values found for structurally similar molecules in the Cambridge Structural Database (CSD Version 5.24; Allen, 2002). Because of the existence of a conjugated system, the N1—C8 [1.314 (2) Å] and N2—C8 [1.301 (2) Å] bond distances are significantly shorter than the typical Csp2—N bond distance (1.426 Å; Lorente et al., 1995). The dihedral angle between the aryl rings and the oxazolidine ring is 2.856 (3)° and the C4—C7—N2—C8 torsion angle is 175.45 (2)°.

An intramolecular N1—H11···O1 hydrogen bond is found and centrosymmetrically related molecules are connected via N—H···O hydrogen bonds involving the same atoms (Table 1).

Related literature top

For related literature, see: Allen (2002); Jiang et al. (2006); Lorente et al. (1995); Zhang et al. (2004).

Experimental top

N-Benzoyl-N'-(2-hydroxy-ethyl)thiourea was reacted with dicyclohexylcarbodiimide under weakly basic conditions in CH3CN to give (I) in 90% yield. Single crystals suitable for the X-ray diffraction study were obtained by slow evaporation of an acetone/water solution of (I).

Refinement top

All the H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H distances of 0.93–0.97 Å and and N—H = 0.86 Å, and with Uiso(H) = 1.2Ueq(carrier atom).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I), showing the atom-numbering scheme and 30% probability displacement ellipsoids.
(E)—N-(1,3-Oxazolidin-2-ylidene)benzamide top
Crystal data top
C10H10N2O2Dx = 1.338 Mg m3
Mr = 190.20Melting point = 411–412 K
Orthorhombic, PccnMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ab 2acCell parameters from 1672 reflections
a = 11.4194 (18) Åθ = 3.3–22.3°
b = 20.590 (3) ŵ = 0.10 mm1
c = 8.0325 (13) ÅT = 293 K
V = 1888.7 (5) Å3Block, colorless
Z = 80.25 × 0.23 × 0.18 mm
F(000) = 800
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
1850 independent reflections
Radiation source: sealed tube1091 reflections with I > 2σ(I)
graphiteRint = 0.095
φ and ω scansθmax = 26.0°, θmin = 2.0°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 814
Tmin = 0.973, Tmax = 0.988k = 2525
9475 measured reflectionsl = 99
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.122 w = 1/[σ2(Fo2) + (0.064P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.91(Δ/σ)max < 0.001
1850 reflectionsΔρmax = 0.15 e Å3
128 parametersΔρmin = 0.13 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0047 (12)
Crystal data top
C10H10N2O2V = 1888.7 (5) Å3
Mr = 190.20Z = 8
Orthorhombic, PccnMo Kα radiation
a = 11.4194 (18) ŵ = 0.10 mm1
b = 20.590 (3) ÅT = 293 K
c = 8.0325 (13) Å0.25 × 0.23 × 0.18 mm
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
1850 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
1091 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.988Rint = 0.095
9475 measured reflectionsθmax = 26.0°
Refinement top
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.122Δρmax = 0.15 e Å3
S = 0.91Δρmin = 0.13 e Å3
1850 reflectionsAbsolute structure: ?
128 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.34177 (19)0.35640 (11)0.2998 (3)0.0796 (7)
H10.31070.34670.19580.096*
C20.33903 (19)0.41901 (11)0.3592 (3)0.0792 (7)
H20.30600.45180.29480.095*
C30.38492 (17)0.43353 (9)0.5133 (2)0.0652 (5)
H30.38240.47600.55230.078*
C40.43460 (15)0.38564 (8)0.6105 (2)0.0518 (5)
C50.43765 (17)0.32282 (9)0.5492 (2)0.0606 (5)
H50.47160.29000.61230.073*
C60.3907 (2)0.30858 (10)0.3953 (3)0.0734 (6)
H60.39230.26610.35610.088*
C70.48292 (16)0.40198 (8)0.7777 (2)0.0539 (5)
C80.58435 (15)0.35996 (8)1.0000 (2)0.0514 (5)
C90.6620 (2)0.39852 (9)1.2444 (2)0.0701 (6)
H9A0.61060.40591.33870.084*
H9B0.73250.42431.25740.084*
C100.69031 (19)0.32699 (9)1.2239 (2)0.0709 (6)
H10A0.77420.32041.21490.085*
H10B0.66110.30211.31770.085*
N10.60390 (14)0.41239 (7)1.08905 (18)0.0630 (5)
H110.57460.44941.06180.076*
N20.53248 (13)0.35040 (7)0.85798 (18)0.0557 (4)
O10.47644 (13)0.45792 (6)0.83169 (16)0.0782 (5)
O20.63240 (12)0.30804 (6)1.07298 (15)0.0702 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0837 (16)0.0822 (17)0.0728 (14)0.0054 (13)0.0193 (12)0.0120 (12)
C20.0868 (16)0.0684 (15)0.0823 (15)0.0118 (12)0.0207 (13)0.0051 (12)
C30.0741 (13)0.0489 (11)0.0725 (12)0.0070 (10)0.0089 (11)0.0020 (10)
C40.0559 (11)0.0425 (10)0.0568 (10)0.0018 (8)0.0024 (9)0.0010 (8)
C50.0740 (13)0.0465 (11)0.0613 (11)0.0053 (9)0.0016 (10)0.0052 (9)
C60.0869 (15)0.0582 (13)0.0749 (13)0.0031 (11)0.0054 (12)0.0148 (10)
C70.0604 (12)0.0413 (10)0.0601 (11)0.0024 (8)0.0036 (9)0.0008 (8)
C80.0566 (11)0.0381 (10)0.0595 (11)0.0041 (8)0.0055 (9)0.0014 (8)
C90.0838 (15)0.0544 (12)0.0723 (13)0.0090 (10)0.0162 (11)0.0075 (10)
C100.0814 (14)0.0557 (12)0.0756 (13)0.0105 (10)0.0195 (11)0.0054 (10)
N10.0832 (12)0.0403 (9)0.0655 (9)0.0110 (8)0.0120 (9)0.0057 (7)
N20.0694 (10)0.0404 (9)0.0572 (9)0.0036 (7)0.0051 (8)0.0042 (7)
O10.1163 (12)0.0400 (8)0.0782 (9)0.0130 (8)0.0197 (8)0.0105 (6)
O20.0925 (10)0.0420 (7)0.0760 (9)0.0129 (6)0.0233 (8)0.0034 (6)
Geometric parameters (Å, °) top
C1—C61.367 (3)C7—N21.365 (2)
C1—C21.375 (3)C8—N21.301 (2)
C1—H10.9300C8—N11.314 (2)
C2—C31.377 (3)C8—O21.3368 (19)
C2—H20.9300C9—N11.442 (2)
C3—C41.380 (2)C9—C101.517 (2)
C3—H30.9300C9—H9A0.9700
C4—C51.384 (2)C9—H9B0.9700
C4—C71.491 (2)C10—O21.435 (2)
C5—C61.379 (2)C10—H10A0.9700
C5—H50.9300C10—H10B0.9700
C6—H60.9300N1—H110.8599
C7—O11.2328 (19)
C6—C1—C2119.4 (2)N2—C8—N1132.76 (16)
C6—C1—H1120.3N2—C8—O2116.77 (15)
C2—C1—H1120.3N1—C8—O2110.42 (16)
C1—C2—C3120.44 (19)N1—C9—C10101.33 (15)
C1—C2—H2119.8N1—C9—H9A111.5
C3—C2—H2119.8C10—C9—H9A111.5
C2—C3—C4120.66 (18)N1—C9—H9B111.5
C2—C3—H3119.7C10—C9—H9B111.5
C4—C3—H3119.7H9A—C9—H9B109.3
C3—C4—C5118.47 (17)O2—C10—C9104.92 (14)
C3—C4—C7120.05 (16)O2—C10—H10A110.8
C5—C4—C7121.48 (16)C9—C10—H10A110.8
C6—C5—C4120.52 (17)O2—C10—H10B110.8
C6—C5—H5119.7C9—C10—H10B110.8
C4—C5—H5119.7H10A—C10—H10B108.8
C1—C6—C5120.6 (2)C8—N1—C9112.72 (15)
C1—C6—H6119.7C8—N1—H11121.5
C5—C6—H6119.7C9—N1—H11125.1
O1—C7—N2125.85 (17)C8—N2—C7119.04 (14)
O1—C7—C4120.36 (16)C8—O2—C10109.99 (14)
N2—C7—C4113.79 (15)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H11···O10.862.172.696 (2)119
N1—H11···O1i0.862.172.8944 (19)142
Symmetry codes: (i) −x+1, −y+1, −z+2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H11···O10.862.172.696 (2)119
N1—H11···O1i0.862.172.8944 (19)142
Symmetry codes: (i) −x+1, −y+1, −z+2.
Acknowledgements top

The author thanks the Department of Science and Technology of Hexi University for financial support.

references
References top

Allen, F. H. (2002). Acta Cryst. B58, 380–388.

Bruker (2000). SMART (Version 5.618), SAINT (Version 6.02), SADABS (Version X.XX) and SHELXTL (Version 6.10). Bruker AXS Inc., Madison, Wisconsin, USA.

Jiang, J. L., Duan, C. X., Li, Y. Z., Bai, J. F. & Pan, Y. (2006). Anal. Sci. 22, x119–x120.

Lorente, A., Galan, C., Fonseea, I. & Sanz-Aparicio, J. (1995). Can. J. Chem. 73, 1546–1555.(Version X.XX)

Zhang, Y. M., Xian, L., Wei, T. B. & Yu, K. B. (2004). or (2003).??? J. Chem. Res. pp. 798–799. Please check date; 2004 in Comment section in CIF.